12,522,538 research outputs found

    Type 1 diabetes

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    Type 1 diabetes is a chronic autoimmune disease characterised by insulin deficiency and resultant hyperglycaemia. Knowledge of type 1 diabetes has rapidly increased over the past 25 years, resulting in a broad understanding about many aspects of the disease, including its genetics, epidemiology, immune and β-cell phenotypes, and disease burden. Interventions to preserve β cells have been tested, and several methods to improve clinical disease management have been assessed. However, wide gaps still exist in our understanding of type 1 diabetes and our ability to standardise clinical care and decrease disease-associated complications and burden. This Seminar gives an overview of the current understanding of the disease and potential future directions for research and care

    An Infrared Comparison of Type-1 and Type-2 Quasars

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    We model the optical to far-infrared SEDs of a sample of six type-1 and six type-2 quasars selected in the mid-infrared. The objects in our sample are matched in mid-IR luminosity and selected based on their Spitzer IRAC colors. We obtained new targeted Spitzer IRS and MIPS observations and used archival photometry to examine the optical to far-IR SEDs. We investigate whether the observed differences between samples are consistent with orientation-based unification schemes. The type-1 objects show significant emission at 3 micron. They do not show strong PAH emission and have less far-IR emission on average when compared to the type-2 objects. The SEDs of the type-2 objects show a wide assortment of silicate features, ranging from weak emission to deep silicate absorption. Some also show strong PAH features. In comparison, silicate is only seen in emission in the type-1 objects. This is consistent with some of the type-2s being reddened by a foreground screen of cooler dust, perhaps in the host galaxy itself. We investigate the AGN contribution to the far-IR emission and find it to be significant. We also estimate the star formation rate for each of the objects by integrating the modeled far-IR flux and compare this with the SFR found from PAH emission. We find the type-2 quasars have a higher average SFR than the type-1 quasars based on both methods, though this could be due to differences in bolometric luminosities of the objects. While we find pronounced differences between the two types of objects, none of them are inconsistent with orientation-based unification schemes.Comment: Accepted for publication in Ap

    SO_0(1,d+1) Racah coefficients: Type I representations

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    We use AdS/CFT inspired methods to study the Racah coefficients for type I representations of the Lorentz group SO_0(1,d+1) with d>1. For such representations (a multiple of) the Racah coefficient can be represented as an integral of a product of 6 bulk-to-bulk propagators over 4 copies of the hyperbolic space H_{d+1}. To compute the integrals we represent the bulk-to-bulk propagators in terms of bulk-to-boundary ones. The bulk integrals can be computed explicitly, and the boundary integrations are carried out by introducing Feynman parameters. The final result is an integral representation of the Racah coefficient given by 4 Barnes-Mellin type integrals.Comment: 20 pages, 1 figure. v2: Case d=1 corrected, case d>1 clarifie

    Type 1 diabetes in children

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    Many children are not diagnosed early enough. Nicky Kime highlights the symptoms and importance of an accurate early diagnosis

    Cluster algebras of type A2(1)A_2^{(1)}

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    In this paper we study cluster algebras \myAA of type A2(1)A_2^{(1)}. We solve the recurrence relations among the cluster variables (which form a T--system of type A2(1)A_2^{(1)}). We solve the recurrence relations among the coefficients of \myAA (which form a Y--system of type A2(1)A_2^{(1)}). In \myAA there is a natural notion of positivity. We find linear bases \BB of \myAA such that positive linear combinations of elements of \BB coincide with the cone of positive elements. We call these bases \emph{atomic bases} of \myAA. These are the analogue of the "canonical bases" found by Sherman and Zelevinsky in type A1(1)A_{1}^{(1)}. Every atomic basis consists of cluster monomials together with extra elements. We provide explicit expressions for the elements of such bases in every cluster. We prove that the elements of \BB are parameterized by \ZZ^3 via their g\mathbf{g}--vectors in every cluster. We prove that the denominator vector map in every acyclic seed of \myAA restricts to a bijection between \BB and \ZZ^3. In particular this gives an explicit algorithm to determine the "virtual" canonical decomposition of every element of the root lattice of type A2(1)A_2^{(1)}. We find explicit recurrence relations to express every element of \myAA as linear combinations of elements of \BB.Comment: Latex, 40 pages; Published online in Algebras and Representation Theory, springer, 201

    Cell Therapy for Type 1 Diabetes

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    Acknowledgements The work described in this review was supported by a grant from the MRC. K.R.M. is supported by a fellowship from the Scottish Translational Medicines and Therapeutics Initiative through the Wellcome Trust.Peer reviewedPublisher PD

    Type Dn(1)D_n^{(1)} rigged configuration bijection

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    We establish a bijection between the set of rigged configurations and the set of tensor products of Kirillov--Reshetikhin crystals of type Dn(1)D^{(1)}_n in full generality. We prove the invariance of rigged configurations under the action of the combinatorial RR-matrix on tensor products and show that the bijection preserves certain statistics (cocharge and energy). As a result, we establish the fermionic formula for type Dn(1)D_n^{(1)}. In addition, we establish that the bijection is a classical crystal isomorphism.Comment: 54 page

    D=4, N=1, Type IIA Orientifolds

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    We study D=4, N=1, type IIA orientifold with orbifold group ZNZ_N and ZN×ZMZ_N \times Z_M. We calculate one-loop vacuum amplitudes for Klein bottle, cylinder and Mobius strip and extract the tadpole divergences. We find that the tadpole cancellation conditions thus obtained are satisfied by the Z4Z_4, Z8Z_8, Z8Z'_8, Z12Z'_{12} orientifolds while there is no solution for Z3Z_3, Z7Z_7, Z6Z_6, Z6Z'_6, Z12Z_{12}. The Z4×Z4Z_4 \times Z_4 type IIA orientifold is also constructed by introducing four different configurations of 6-branes. We argue about perturbative versus non-perturbative orientifold vacua under T- duality between the type IIA and the type IIB ZNZ_N orientifolds in four dimensions.Comment: 32 pages, LaTe
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